Download presentation

1
**Matrix Representation**

Matrix Rep. Same basics as introduced already. Convenient method of working with vectors. Superposition Complete set of vectors can be used to express any other vector. Complete set of N vectors can form other complete sets of N vectors. Can find set of vectors for Hermitian operator satisfying Eigenvectors and eigenvalues Matrix method Find superposition of basis states that are eigenstates of particular operator. Get eigenvalues. Copyright – Michael D. Fayer, 2007

2
**Orthonormal basis set in N dimensional vector space**

basis vectors Any vector can be written as with To get this, project out Copyright – Michael D. Fayer, 2007

3
**Substituting the series in terms of bases vectors.**

Operator equation Substituting the series in terms of bases vectors. Left mult. by The N2 scalar products are completely determined by N values of j ; N for each yi Copyright – Michael D. Fayer, 2007

4
**Matrix elements of A in the basis**

Writing Matrix elements of A in the basis gives for the linear transformation Know the aij because we know A and In terms of the vector representatives (Set of numbers, gives you vector when basis is known.) vector vector representative, must know basis The set of N linear algebraic equations can be written as double underline means matrix Copyright – Michael D. Fayer, 2007

5
**array of coefficients - matrix**

The aij are the elements of the matrix The product of matrix and vector representative x is a new vector representative y with components Copyright – Michael D. Fayer, 2007

6
**Matrix Properties, Definitions, and Rules**

Two matrices, and are equal if aij = bij. The unit matrix ones down principal diagonal Gives identity transformation Corresponds to The zero matrix Copyright – Michael D. Fayer, 2007

7
**Matrix multiplication**

Consider operator equations Using the same basis for both transformations has elements Law of matrix multiplication Example Copyright – Michael D. Fayer, 2007

8
**Multiplication Associative**

Multiplication NOT Commutative Matrix addition and multiplication by complex number Inverse of a matrix inverse of identity matrix transpose of cofactor matrix (matrix of signed minors) determinant Copyright – Michael D. Fayer, 2007

9
**interchange rows and columns Transpose**

Reciprocal of Product For matrix defined as interchange rows and columns Transpose Complex Conjugate complex conjugate of each element Hermitian Conjugate complex conjugate transpose Copyright – Michael D. Fayer, 2007

10
**transpose of product is product of transposes in reverse order**

Rules transpose of product is product of transposes in reverse order determinant of transpose is determinant complex conjugate of product is product of complex conjugates determinant of complex conjugate is complex conjugate of determinant Hermitian conjugate of product is product of Hermitian conjugates in reverse order determinant of Hermitian conjugate is complex conjugate of determinant Copyright – Michael D. Fayer, 2007

11
**Definitions Symmetric Hermitian Real Imaginary Unitary Diagonal**

Powers of a matrix Copyright – Michael D. Fayer, 2007

12
**Column vector representative one column matrix**

then vector representatives in particular basis becomes row vector transpose of column vector transpose Hermitian conjugate Copyright – Michael D. Fayer, 2007

13
**Change of Basis orthonormal basis then**

Superposition of can form N new vectors linearly independent a new basis complex numbers Copyright – Michael D. Fayer, 2007

14
**New Basis is Orthonormal**

if the matrix coefficients in superposition meets the condition is unitary Important result. The new basis will be orthonormal if , the transformation matrix, is unitary (see book and Errata and Addenda ). Copyright – Michael D. Fayer, 2007

15
**Same vector – different basis. **

Unitary transformation substitutes orthonormal basis for orthonormal basis Vector Same vector – different basis. vector – line in space (may be high dimensionality abstract space) written in terms of two basis sets The unitary transformation can be used to change a vector representative of in one orthonormal basis set to its vector representative in another orthonormal basis set. x – vector rep. in unprimed basis x' – vector rep. in primed basis change from unprimed to primed basis change from primed to unprimed basis Copyright – Michael D. Fayer, 2007

16
**Vector - line in real space.**

Example Consider basis Vector line in real space. In terms of basis Vector representative in basis Copyright – Michael D. Fayer, 2007

17
**Change basis by rotating axis system 45° around .**

Can find the new representative of , s' is rotation matrix For 45° rotation around z Copyright – Michael D. Fayer, 2007

18
**vector representative of in basis**

Then vector representative of in basis Same vector but in new basis. Properties unchanged. Example – length of vector Copyright – Michael D. Fayer, 2007

19
**Can go back and forth between representatives of a vector by**

change from unprimed to primed basis change from primed to unprimed basis components of in different basis Copyright – Michael D. Fayer, 2007

20
**Consider the linear transformation**

operator equation In the basis can write or Change to new orthonormal basis using or with the matrix given by Because is unitary Copyright – Michael D. Fayer, 2007

21
**Similarity Transformation**

Extremely Important Can change the matrix representing an operator in one orthonormal basis into the equivalent matrix in a different orthonormal basis. Called Similarity Transformation Copyright – Michael D. Fayer, 2007

22
**Relations unchanged by change of basis.**

In basis Go into basis Relations unchanged by change of basis. Example Can insert between because Therefore Copyright – Michael D. Fayer, 2007

23
**Isomorphism between operators in abstract vector space and matrix representatives.**

Because of isomorphism not necessary to distinguish abstract vectors and operators from their matrix representatives. The matrices (for operators) and the representatives (for vectors) can be used in place of the real things. Copyright – Michael D. Fayer, 2007

24
**Hermitian Operators and Matrices**

Hermitian operator Hermitian Matrix + - complex conjugate transpose - Hermitian conjugate Copyright – Michael D. Fayer, 2007

25
**Theorem (Proof: Powell and Craseman, P**

Theorem (Proof: Powell and Craseman, P. 303 – 307, or linear algebra book) For a Hermitian operator A in a linear vector space of N dimensions, there exists an orthonormal basis, relative to which A is represented by a diagonal matrix The vectors, , and the corresponding real numbers, ai, are the solutions of the Eigenvalue Equation and there are no others. Copyright – Michael D. Fayer, 2007

26
**Application of Theorem**

Operator A represented by matrix in some basis The basis is any convenient basis. In general, the matrix will not be diagonal. There exists some new basis eigenvectors in which represents operator and is diagonal eigenvalues. To get from to unitary transformation. Similarity transformation takes matrix in arbitrary basis into diagonal matrix with eigenvalues on the diagonal. Copyright – Michael D. Fayer, 2007

27
Matrices and Q.M. Previously represented state of system by vector in abstract vector space. Dynamical variables represented by linear operators. Operators produce linear transformations. Real dynamical variables (observables) are represented by Hermitian operators. Observables are eigenvalues of Hermitian operators. Solution of eigenvalue problem gives eigenvalues and eigenvectors. Copyright – Michael D. Fayer, 2007

28
**Matrix Representation**

Hermitian operators replaced by Hermitian matrix representations. In proper basis, is the diagonalized Hermitian matrix and the diagonal matrix elements are the eigenvalues (observables). A suitable transformation takes (arbitrary basis) into (diagonal – eigenvector basis) Diagonalization of matrix gives eigenvalues and eigenvectors. Matrix formulation is another way of dealing with operators and solving eigenvalue problems. Copyright – Michael D. Fayer, 2007

29
**All rules about kets, operators, etc. still apply.**

Example Two Hermitian matrices can be simultaneously diagonalized by the same unitary transformation if and only if they commute. All ideas about matrices also true for infinite dimensional matrices. Copyright – Michael D. Fayer, 2007

30
**Example – Harmonic Oscillator**

Have already solved – use occupation number representation kets and bras (already diagonal). matrix elements of a Copyright – Michael D. Fayer, 2007

31
**Copyright – Michael D. Fayer, 2007**

32
**Copyright – Michael D. Fayer, 2007**

33
**Adding the matrices and and multiplying by ½ gives**

The matrix is diagonal with eigenvalues on diagonal. In normal units the matrix would be multiplied by This example shows idea, but not how to diagonalize matrix when you don’t already know the eigenvectors. Copyright – Michael D. Fayer, 2007

34
**matrix representing operator representative of eigenvector**

Diagonalization Eigenvalue equation eigenvalue matrix representing operator representative of eigenvector In terms of the components This represents a system of equations We know the aij. We don't know a - the eigenvalues ui - the vector representatives, one for each eigenvalue. Copyright – Michael D. Fayer, 2007

35
**Besides the trivial solution**

A solution only exists if the determinant of the coefficients of the ui vanishes. know aij, don't know a's Expanding the determinant gives Nth degree equation for the the unknown a's (eigenvalues). Then substituting one eigenvalue at a time into system of equations, the ui (eigenvector representatives) are found. N equations for u's gives only N - 1 conditions. Use normalization. Copyright – Michael D. Fayer, 2007

36
**Example - Degenerate Two State Problem**

Basis - time independent kets orthonormal. a and b not eigenkets. Coupling g. These equations define H. The matrix elements are And the Hamiltonian matrix is Copyright – Michael D. Fayer, 2007

37
**The corresponding system of equations is**

These only have a solution if the determinant of the coefficients vanish. Ground State E = 0 E0 2g Excited State Dimer Splitting Expanding Energy Eigenvalues Copyright – Michael D. Fayer, 2007

38
**To obtain Eigenvectors Use system of equations for each eigenvalue.**

Eigenvectors associated with l+ and l-. and are the vector representatives of and in the We want to find these. Copyright – Michael D. Fayer, 2007

39
**First, for the eigenvalue write system of equations.**

Matrix elements of The matrix elements are The result is Copyright – Michael D. Fayer, 2007

40
**An equivalent way to get the equations is to use a matrix form.**

Substitute Multiplying the matrix by the column vector representative gives equations. Copyright – Michael D. Fayer, 2007

41
**The two equations are identical.**

Always get N – 1 conditions for the N unknown components. Normalization condition gives necessary additional equation. Then and Eigenvector in terms of the basis set. Copyright – Michael D. Fayer, 2007

42
**using the matrix form to write out the equations**

For the eigenvalue using the matrix form to write out the equations Substituting These equations give Using normalization Therefore Copyright – Michael D. Fayer, 2007

43
**Can diagonalize by transformation**

diagonal not diagonal Transformation matrix consists of representatives of eigenvectors in original basis. complex conjugate transpose Copyright – Michael D. Fayer, 2007

44
**after matrix multiplication**

Then Factoring out after matrix multiplication more matrix multiplication diagonal with eigenvalues on diagonal Copyright – Michael D. Fayer, 2007

Similar presentations

© 2020 SlidePlayer.com Inc.

All rights reserved.

To make this website work, we log user data and share it with processors. To use this website, you must agree to our Privacy Policy, including cookie policy.

Ads by Google